Tube lens unit with chromatically compensating effect

ABSTRACT

The invention relates to a tubular lens unit that obtains a chromatically compensating effect when used with objectives having an infinite image distance and chromatic residual errors. The inventive tubular lens unit fulfils the following conditions: equation (1) CHL=CHL o −A &amp;Tgr;   2  m T  &amp;phiv; T =0, and equation (2) CHV=CHV o −1000&amp;1gr; m T  &amp;phiv; T  d 1 =0, wherein CHL represents the chromatic longitudinal deviation of the tubular lens unit, CHL o  represents the chromatic longitudinal deviation of the objective, CHV represents the chromatic magnification difference of the tubular lens unit, CHV o  represents the chromatic magnification difference of the objective, &amp;1gr; represents the wavelength, m T  represents the dispersion index of the tubular lens unit from m &amp;Tgr; =m e =1/&amp;1gr;v wherein e is the main colour index, and &amp;1gr; the Abbe number, A represents the field point, d 1  represents the distance between the first optical element of the tubular lens unit and the entrance pupil, &amp;phiv; &amp;Tgr;  represents the refractive power, and &amp;phiv; T  represents the index of the respective lens in the tubular lens unit.

CROSS REFERENCE TO RELATED PATENT APPLICATIONS

This application is a continuation-in-part of copending international patent application PCT/EP2005/001798 entitled “Tubular Lens Unit Having a Chromatically Compensating Effect” filed Feb. 22, 2005, which claims priority to German Patent Application No. 10 2004 009 848.4, filed Feb. 28, 2004. The entire disclosures of the prior applications are considered as being part of the disclosure of this application and are hereby incorporated by reference herein.

FIELD OF THE INVENTION

The invention relates to a tube lens unit that provides a chromatically compensating effect when used with objectives having an infinite image distance and chromatic residual errors. The tube lens unit is particularly suitable for generating a color-free primary (intermediate) image in the imaging ray paths of microscopes.

BACKGROUND OF THE INVENTION

In prior art, so-called ICS systems (“infinity color-corrected systems”) are known, which consist essentially of an objective having chromatic residual errors and an infinite image distance, and a tube lens unit having a chromatically compensating effect. Thanks to such a combination, the intermediate image, despite the chromatic residual errors of the objective, is formed without chromatic aberrations, so that a very largely true-to-color rendition of microscopic specimen details is obtained throughout the image field.

A considerable disadvantage of the ICS systems known so far is the fact that the distance between the objective and the tube lens unit is variable within close limits only, so that these ICS systems are tied to given tube focal length and thus can only be use with instruments for which they have been conceived.

Frequently, however, it is desirable for the user, for cost reasons, to have a tube lens unit that can be used alternatingly with several optical instruments, each of which was originally conceived for a separate, fixed focal length.

SUMMARY OF THE INVENTION

The invention is therefore based on the problem to create a tube lens unit of the kind mentioned in the beginning, which can be employed with several optical instruments of different tube focal lengths, while always having the same chromatically compensating effect.

This problem is solved by means of a tube lens unit that fulfils the following conditions: CHL=CHL _(o) −A _(T) ² m _(T) φ_(T)=0   Equation (1) CHV=CHV _(o)−1000λm _(T) φ_(T) d ₁=0   Equation (2) where

-   -   CHL is the longitudinal chromatic aberration of the tube lens         unit,     -   CHL_(o) is the longitudinal chromatic aberration of the         objective,     -   CHV is the chromatic difference of magnification of the tube         lens unit,     -   CHV_(o) is the chromatic difference of magnification of the         objective,     -   λ is the wavelength,     -   m_(T) is the dispersion index of the tube lens unit, derived         from m_(T)=m_(e)=1/λν, in which e is the index of the main color         and ν the Abbe number,     -   A_(T) is the radius of the exit pupil of the objective=entrance         pupil of the tube lens unit,     -   A_(T) ² m_(T) φ_(T)=CHL_(T) (longitudinal chromatic aberration         of the tube lens unit),     -   1000λ m_(T) φ_(T) d₁=CHV_(T) (chromatic difference of         magnification of the tube lens unit),     -   d₁ is the distance of the first optical element of the tube lens         unit from the entrance pupil,     -   φ_(T) is the refractive power, and     -   T is the index of the respective lens in the tube lens unit.

For both equations, the product of the values of m_(T) and φ_(T) should have the same amount.

The CHL is given in terms of Rayleigh units RU, and the CHV in terms of 0/00. By normalization to Rayleigh units (1 RU=λ/n sin u), the CHL to be compensated has an aperture-adapted value for objectives and, consequently, also for tube lens units of any focal length. The CHV given in terms of 0/00 must have a constant value for tube lens units of any focal length. (Literature: H. G. Zimmer, Geometrische Optik, Springer Verlag Berlin, Heidelberg, New York.)

The tube lens units must have at least one lens as a compensating optical element. In developments of the invention, however, two or more lenses may be provided as compensating optical elements.

If two lenses are provided, both may be configured as biconvex lenses. Alternatively, one biconvex lens and one cemented component may be provided, the cemented component preferably comprising one biconcave and one planoconvex lens. The plane surface should be arranged facing the eyepiece. In further development versions of the tube lens unit according to the invention, the use of several cemented components is feasible as well.

In embodiments of the optical tube lens unit according to the invention, two cases must be distinguished in principle.

In a first case A, the conditions given by equations (1) and (2) are fulfilled by means of two optical elements, each of which may be a single lens or a cemented component.

The compensating effect is obtained for different magnifications, by the combination of any ICS objectives with the tube lens unit according to the invention, provided the optical elements of the latter have focal lengths of, e.g., 1.3 f, 1 f, 0.8 f, . . . 0.25 f.

Let K₁=−A_(T) ², K₂=1000λ d₁, where K₁₁ and K₁₂ are coefficients of the first optical element and K₂₁ and K₂₂ coefficients of the second optical element; the necessary individual focal lengths of the two elements are derived from the ray coordinates of the aperture and field rays after ray tracing with the various focal lengths of the tube lens unit.

The dispersion indices m₁ and m₂ of the optical elements are determined by K ₁₁ φ₁ m ₁ +K ₁₂ φ₂ m ₂ =−CHL _(o),   Equation (3) and K ₂₁ φ₁ m ₁ +K ₂₂ φ₂ m ₂ =−CHV _(o),   Equation (4) the values of K₁₁, K₁₂, K₂₁ and K₂₂ being determined from ray tracing with φ_(i).

In a second case B, the conditions given by equations (1) and (2) are fulfilled by means of a single lens. Here, the required quantities can be derived from equations (3) and (4), if we set φ₁=φ_(T) and φ₂=0. This makes K₁₁=−A_(T) ², and K₂=1000λ d₁.

Because of the limits for the dispersion indices m_(T), which are between 20 and 90, tube lens units using only a single compensating lens are only possible with limited focal lengths, too. For focal lengths exceeding the limit, a cemented component has to be used also in case B.

For this, the following conditions apply: K ₁ m _(T) φ_(T) =−CHL,   Equation (5) and K ₂ m _(T) φ_(T) =−CHV,   Equation (6) with m_(T)=−CHL/K₁ φ_(T). The value of CHV (=K₂/K₁·CHL) also results therefrom.

The special case B has already been implemented in connection with tube lenses having a focal length of f=160 mm.

The solution according to the invention has made it basically possible to use also such optical elements (lenses) in the tube lens unit whose focal length f considerably deviates from the value of f=160 mm as common so far.

It has further been discovered that known technical glass, e.g., SF6, can be used for compensating optical elements in the tube lens having a focal length of 350 mm. In this way it is possible to achieve that all ICS objectives having chromatic residual errors of CHL_(o)=+5.7 [RU] and CHV_(o)=+14.2 [0/00] can be used for an ICS optical system.

DESCRIPTION OF THE FIGURES

Below, the invention is explained in more detail, going by two exemplary embodiments, wherein

FIG. 1 shows a tube lens unit according to case A featuring a single lens and a cemented component consisting of a biconcave and a planoconvex lens,

FIG. 2 shows a tube lens unit according to case B featuring a single lens, and

FIG. 3 shows another tube lens unit according to case A, but featuring two cemented components.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

FIG. 1 shows the principle of the embodiment of a tube lens unit TL according to case A. Beginning on the left-hand margin, the drawing contains the following details: the optical axis 1; the position 2 of the entrance pupil of an objective (not shown by the drawing); a first lens 3 arranged at a distance d₁=126 mm from position 2, as a compensating optical element having the thickness d₂=6 mm and the radii r₃₁=62.634 mm and r₃₂=−117.15 mm; a cemented component following at a distance d₃=25.1 mm as a second compensating optical element, consisting of a biconcave lens 4 having a thickness d₄=2 mm and the radii r₄₁=−55.033 mm and r₄₂=49.048 mm, and a planoconvex lens 5 having the thickness d₅=3.5 mm and the radii r₅₁=49.048 mm and r₅₂=∞. The distance between the planoconvex lens 5 of the cemented component and the intermediate image plane 7 is d₆=167 mm.

The entrance pupil of the objective of infinite image distance, the chromatic residual error of which is to be compensated by means of the tube lens unit TL shown, is in position 2.

The glasses intended are N-PK51 for lens 3, N-LAK10 for lens 4, and N-SF5 for lens 5.

FIG. 2 shows an exemplary embodiment of a tube lens unit TL according to the case B described above.

Beginning on the left-hand margin, the drawing contains the following details: the optical axis 1; the position 2 of the entrance pupil of an objective (not shown by the drawing); a first lens 6 arranged at a distance d₇=126 mm and having a thickness d₈=10.9 mm and the radii r₆₁=189.417 mm and r₆₂=−189.417 mm. The distance between the lens 6 and the intermediate image plane 7 is d₉=167 mm. Here again, the objective of infinite image distance, the chromatic residual error of which is to be compensated by means of the tube lens unit TL shown, is not shown by the drawing. The entrance pupil of this objective is in position 2.

Lens 6 is made of technical N-BaLF4 glass.

FIG. 3 shown another possible embodiment of the tube lens unit TL according to the invention and to case A. Here again, the drawing shows the optical axis 1, the position 2 of the entrance pupil of an objective (not shown by the drawing), and the intermediate image plane 7.

Other than in the embodiment shown in FIG. 1, this version is provided with two cemented components as compensating optical elements, with the first cemented components consisting of two lenses 8 and 9, and the other cemented component consisting of two lenses 10 and 11.

Lens 8 is made of N-PSK 53 glass and has a thickness d₁₁=4 mm and radii r₈₁=23.714 mm and r₈₂=−37.584 mm. Lens 9 is made of N-LASF45 glass and has a thickness d₁₂=2 mm and radii r₉₁=−37.584 mm and r₉₂=−375.84 mm.

Lens 10 in the second cemented component consists of technical N-FK5 glass and has a thickness of d₁₄=1.5 mm and radii of r₁₀₁=−10.593 mm and r₁₀₂=6.13 mm. The material intended for lens 11 is N-LASF45, its thickness is d₁₅=2.5 mm, and its radii are r₁₁₁=6.13 mm and r₁₁₂=8.9125 mm.

The distance between the position 2 of the entrance pupil and the first cemented component is d₁₀=126 mm, the distance between the two cemented components is d₁₃=25.82 mm, and the distance between the second component and the intermediate image plane 7 is d₁₆=167 mm.

The problem of the invention, i.e. the provision of a tube lens unit TL that can be used with a good chromatically compensating effect for several optical instruments having different tube focal lengths, is solved by using suitable focal lengths and glass materials for the elements of the tube lens unit TL, which contains different focal lengths.

LIST OF REFERENCE NUMBERS

-   1 Optical axis -   2 Position of the entrance pupil of an objective -   3 Lens -   4 Lens -   5 Lens -   6 Lens -   7 Intermediate image plane -   8 Lens -   9 Lens -   10 Lens -   11 Lens -   TL Tube lens unit -   d_(ij) Distances and thicknesses -   r_(ij) Radii 

1. A tube lens unit, containing various focal lengths, with chromatically compensating effect for use with objectives of infinite image distance and chromatic residual errors, characterized in that the tube lens unit (TL) satisfies the following conditions: CHL=CHL _(o) −A _(T) ² m _(T) φ_(T)=0   Equation (1) CHV=CHV _(o)−1000λm _(T) φ_(T) d ₁=0   Equation (2)  where CHL is the longitudinal chromatic aberration of the combination of tube lens unit plus objective, CHL_(o) is the longitudinal chromatic aberration of the objective, CHV is the chromatic difference of magnification of the combination of tube lens unit plus objective, CHV_(o) is the chromatic difference of magnification of the objective, λ is the wavelength, m_(T) is the dispersion index of the optical elements in the tube lens unit (TL), derived from m_(T)=m_(e)=1/λν, in which e is the index of the main color and ν the Abbe number, A_(T) is the radius of the exit pupil of the objective=entrance pupil of the tube lens unit, d₁ is the distance of the first optical element of the tube lens unit (TL) from the entrance pupil, φ_(T) is the refractive power, and T is the index of the respective lens in the tube lens unit (TL), A_(T) ² m_(T) φ_(T)=CHL_(T) is the longitudinal chromatic aberration of the tube lens unit, and 1000λ_(e) m_(T) φ_(T) d₁=CHV_(T) is the chromatic difference of magnification of the tube lens unit.
 2. A tube lens unit as claimed in claim 1, characterized in that at least one compensating optical element is provided, which, allowing for equations (1) and (2), is determined by K ₁₁ φ₁ m ₁ +K ₁₂ φ₂ m ₂=−CHL_(o),   Equation (3) and K ₂₁ φ₁ m ₁ +K ₂₂ φ₂ m ₂ =−CHV _(o),   Equation (4) the values of K₁₁, K₁₂, K₂₁ and K₂₂ being coefficients determined from ray tracing with φ_(i).
 3. A tube lens unit as claimed in claim 2, characterized in that one compensating optical element is provided, which is configured as a biconvex lens.
 4. A tube lens unit as claimed in claim 2, characterized in that two compensating optical elements are provided, a first of which is configured as a biconvex lens and the second one as a cemented component.
 5. A tube lens unit as claimed in claim 4, characterized in that the cemented component comprises a biconvex and a planoconvex lens, with the plane surface arranged to face the eyepiece.
 6. A tube lens unit as claimed in claim 2, characterized in that two compensating optical elements are provided and both are configured as cemented components. 